<p>We develop a finite-<i>N</i> matched-asymptotic theory for Smoluchowski coagulation. Starting from the infinite system of ODEs, we use conservation laws to obtain closed scalar evolution equations for suitable moments. For the constant kernel <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math> <msub> <mi>a</mi> <mrow> <mi>j</mi> <mo>,</mo> <mi>k</mi> </mrow> </msub> <mo>=</mo> <mi>K</mi> </math></EquationSource> <EquationSource Format="TEX">$a_{j,k}=K$</EquationSource> </InlineEquation>, this leads to an exact early-time decay law for the cluster number and the linear coalescence-time scaling <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <mi>N</mi> </msub> <mo>≍</mo> <mi>N</mi> </math></EquationSource> <EquationSource Format="TEX">$T_{N}\asymp N$</EquationSource> </InlineEquation> when the volume scales as <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math> <mi>V</mi> <mo>∼</mo> <mi>N</mi> </math></EquationSource> <EquationSource Format="TEX">$V\sim N$</EquationSource> </InlineEquation>. For the sum kernel <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math> <msub> <mi>a</mi> <mrow> <mi>j</mi> <mo>,</mo> <mi>k</mi> </mrow> </msub> <mo>=</mo> <mi>j</mi> <mo>+</mo> <mi>k</mi> </math></EquationSource> <EquationSource Format="TEX">$a_{j,k}=j+k$</EquationSource> </InlineEquation>, the same reduction yields an exponential decay regime for the number of clusters and a logarithmic finite-<i>N</i> coalescence time. For the multiplicative kernel <InlineEquation ID="IEq5"> <EquationSource Format="MATHML"><math> <msub> <mi>a</mi> <mrow> <mi>j</mi> <mo>,</mo> <mi>k</mi> </mrow> </msub> <mo>=</mo> <mi>j</mi> <mi>k</mi> </math></EquationSource> <EquationSource Format="TEX">$a_{j,k}=jk$</EquationSource> </InlineEquation>, we recover the classical finite-time blowup of the second moment and show that finite <i>N</i> produces a sharp gelation cutoff preceding the mean-field gelation time by a window of order <InlineEquation ID="IEq6"> <EquationSource Format="MATHML"><math> <msup> <mi>N</mi> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">$N^{-2}$</EquationSource> </InlineEquation>. In all kernels considered, the late-time dynamics involve only finitely many clusters and contribute only lower-order corrections. The resulting structure closely parallels that of finite-<i>N</i> two-species annihilation: a conserved quantity reduces the dynamics to a scalar ODE, asymptotic matching at a characteristic time yields the finite-size scaling laws, and post-matching effects do not alter the leading behaviour.</p>

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Finite–N scaling, gelation cutoff, and matched asymptotics for Smoluchowski coagulation equation

  • Varun Kumar,
  • Saiful R. Mondal

摘要

We develop a finite-N matched-asymptotic theory for Smoluchowski coagulation. Starting from the infinite system of ODEs, we use conservation laws to obtain closed scalar evolution equations for suitable moments. For the constant kernel a j , k = K $a_{j,k}=K$ , this leads to an exact early-time decay law for the cluster number and the linear coalescence-time scaling T N N $T_{N}\asymp N$ when the volume scales as V N $V\sim N$ . For the sum kernel a j , k = j + k $a_{j,k}=j+k$ , the same reduction yields an exponential decay regime for the number of clusters and a logarithmic finite-N coalescence time. For the multiplicative kernel a j , k = j k $a_{j,k}=jk$ , we recover the classical finite-time blowup of the second moment and show that finite N produces a sharp gelation cutoff preceding the mean-field gelation time by a window of order N 2 $N^{-2}$ . In all kernels considered, the late-time dynamics involve only finitely many clusters and contribute only lower-order corrections. The resulting structure closely parallels that of finite-N two-species annihilation: a conserved quantity reduces the dynamics to a scalar ODE, asymptotic matching at a characteristic time yields the finite-size scaling laws, and post-matching effects do not alter the leading behaviour.